“…The larger particles of this distribution correspond to polydispersed primary particles, with properties that depend upon both the radial and axial position within the flame, and that ultimately lead to a distribution with a mean radius of gyration, <R g >, of 21 nm and a polydispersity, σ S /<R g >, of 0.2, where σ S is the width of the Schultz distribution [14]. The smaller particles, which require additional experiments before they can be identified, may be the soot nuclei observed by di Stasio [15], a polycyclic aromatic hydrocarbon such as naphthalene, which we have observed [16], and/or disordered carbons with graphitic basal planes observed by Chen and Dobbins [17]. the Porod region, the scattering intensity scales as 1/q 4 and, if the system is not too polydispersed, interference fringes may be observed that will directly provide <R g > and the polydispersity, σ/<R g >, where σ is the width of the distribution.…”